EP2374205B1 - Piezoelektrische quasi-resonanzmotoren auf der basis von akustischen stehwellen mit kombiniertem resonator - Google Patents

Piezoelektrische quasi-resonanzmotoren auf der basis von akustischen stehwellen mit kombiniertem resonator Download PDF

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Publication number
EP2374205B1
EP2374205B1 EP09838002.5A EP09838002A EP2374205B1 EP 2374205 B1 EP2374205 B1 EP 2374205B1 EP 09838002 A EP09838002 A EP 09838002A EP 2374205 B1 EP2374205 B1 EP 2374205B1
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Prior art keywords
piezoresonator
piezoelectric device
along
electrodes
contact elements
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English (en)
French (fr)
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EP2374205A4 (de
EP2374205A2 (de
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Serhiy Petrenko
Valentin Rangelov Zhelyaskov
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Discovery Technology International Inc
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Discovery Technology International Inc
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    • H—ELECTRICITY
    • H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N30/00—Piezoelectric or electrostrictive devices
    • H10N30/20—Piezoelectric or electrostrictive devices with electrical input and mechanical output, e.g. functioning as actuators or vibrators
    • H10N30/202—Piezoelectric or electrostrictive devices with electrical input and mechanical output, e.g. functioning as actuators or vibrators using longitudinal or thickness displacement combined with bending, shear or torsion displacement
    • H10N30/2027—Piezoelectric or electrostrictive devices with electrical input and mechanical output, e.g. functioning as actuators or vibrators using longitudinal or thickness displacement combined with bending, shear or torsion displacement having cylindrical or annular shape
    • H—ELECTRICITY
    • H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02N—ELECTRIC MACHINES NOT OTHERWISE PROVIDED FOR
    • H02N2/00—Electric machines in general using piezoelectric effect, electrostriction or magnetostriction
    • H02N2/0005—Electric machines in general using piezoelectric effect, electrostriction or magnetostriction producing non-specific motion; Details common to machines covered by H02N2/02 - H02N2/16
    • H02N2/001—Driving devices, e.g. vibrators
    • H02N2/002—Driving devices, e.g. vibrators using only longitudinal or radial modes
    • H02N2/0025—Driving devices, e.g. vibrators using only longitudinal or radial modes using combined longitudinal modes
    • H—ELECTRICITY
    • H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02N—ELECTRIC MACHINES NOT OTHERWISE PROVIDED FOR
    • H02N2/00—Electric machines in general using piezoelectric effect, electrostriction or magnetostriction
    • H02N2/02—Electric machines in general using piezoelectric effect, electrostriction or magnetostriction producing linear motion, e.g. actuators; Linear positioners ; Linear motors
    • H02N2/026—Electric machines in general using piezoelectric effect, electrostriction or magnetostriction producing linear motion, e.g. actuators; Linear positioners ; Linear motors by pressing one or more vibrators against the driven body
    • H—ELECTRICITY
    • H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02N—ELECTRIC MACHINES NOT OTHERWISE PROVIDED FOR
    • H02N2/00—Electric machines in general using piezoelectric effect, electrostriction or magnetostriction
    • H02N2/10—Electric machines in general using piezoelectric effect, electrostriction or magnetostriction producing rotary motion, e.g. rotary motors
    • H02N2/103—Electric machines in general using piezoelectric effect, electrostriction or magnetostriction producing rotary motion, e.g. rotary motors by pressing one or more vibrators against the rotor
    • H—ELECTRICITY
    • H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N30/00—Piezoelectric or electrostrictive devices
    • H10N30/20—Piezoelectric or electrostrictive devices with electrical input and mechanical output, e.g. functioning as actuators or vibrators
    • H10N30/206—Piezoelectric or electrostrictive devices with electrical input and mechanical output, e.g. functioning as actuators or vibrators using only longitudinal or thickness displacement, e.g. d33 or d31 type devices

Definitions

  • the invention relates to piezoelectric motors, and more particularly to piezoelectric quasi-resonance motors based on standing acoustic waves and a combined resonator.
  • This configuration generally enables a plane longitudinal elastic 2-D wave to be excited in the piezoelectric element.
  • the result is generally the linear displacement of the contact point, which is typically located in the center of the resonator and is coupled to the rest of the motor using a contact or friction element attached to the surface of the piezoelectric element.
  • U.S. Patent No. 5,665,918 discloses a linear vibration actuator which obtains a driving force from two simultaneously produced planar standing waves causing driving pieces to perform elliptic motions.
  • the various embodiments of the present invention provide a new piezoelectric motor.
  • the new piezoelectric motor is a resonance-type piezoelectric motor using standing acoustic waves.
  • the new piezoelectric motor operates by providing high efficiency nano-elliptical motion at different contact points on the piezoelectric element to provide lateral motion or the piezoelement or the stage, as described below.
  • the high efficiency of this new piezoelectric motor stems from the fact that when the contact points are acting on the moving stage, the contact points are moving along the top portion of a relatively flat elliptical path. Therefore, a substantial portion of the force applied by the contact points against the stage is in a direction generally parallel to the direction of motion.
  • the nano-elliptical motion at a contact point is provided by the superposition of two orthogonal standing waves, as opposed to a single plane wave. As a result, excitation of higher order modes can be performed and a large number of contact points can be provided for the actuator.
  • Resonant piezoelectric motors with standing acoustic waves create motion from rotational deformations. These rotational deformations are generally in the form of very small nano-ellipses.
  • nano-ellipses of rotational movement must be established with similar or corresponding directions of rotational deformation.
  • the elliptical rotations are generally in the first rotational direction to provide linear movement in a first linear direction.
  • the elliptical rotations are generally in a second rotational direction, opposite to the first rotational direction, to provide linear movement in the first linear direction.
  • a piezoresonator in accordance with an embodiment of the invention includes electrodes and leads coupled to opposite sides of the piezoresonator for excitation of longitudinal vibrations, in particular standing acoustic waves.
  • the longitudinal vibrations cause motion of contact sites, which interact by friction with guides through contact elements on upper and lower surfaces of the piezoresonator.
  • the contact elements are integrally formed with the piezoresonator.
  • the piezoresonator can be held against the guides under pressure provided by a pressure-creating device, such as spring.
  • the contact sites are situated at the place of maximum vibrational velocity of the resonator.
  • the size of the piezoresonator and the locations of the electrodes are selected to satisfy the conditions for simultaneous formation of higher order longitudinal vibrational modes in a first direction of the piezoresonator along the length of the piezoresonator and conditions for excitation of a first order longitudinal vibrational mode in a second direction along the width of the piezoresonator.
  • the natural frequencies (resonant frequencies) along the first and second directions are different and an alternating voltage source having a frequency between the natural frequencies along the first and second directions is used for exciting the piezoresonator during forward or reverse motion.
  • the exemplary piezoelectric actuators (100, 125, 150, 175) each comprise a piezoresonator (3) and contact elements (5).
  • the exemplary piezoelectric actuators (100, 125, 150) also comprise guides (2) and a spring (1).
  • excitation of the piezoresonator (3) in accordance with an embodiment of the present invention causes motion of the contact elements (5) along a nano-elliptical paths (12, 13).
  • the elliptical paths (12, 13) have amplitudes (i.e. dimensions of the minor and major axes) on the order of tens to hundreds of nanometers and are generally flat with respect to the direction of motion.
  • the major axis of the resulting elliptical paths (12, 13) is generally located in a direction parallel to the direction of motion.
  • the contact elements (5) When the contact elements (5) are at a point along the elliptical paths (12, 13) furthest in from the piezoelement, they interact by friction with the guides (2) to initiate a linear micro-motion of the piezoresonator (3) in respect to guides (2).
  • Spring (1) provides a normal force to piezoresonator (3) and guides (2) to assure an adequate friction force.
  • the contact elements (5) are at a point along the elliptical paths (12, 13) closest to the piezoresonator (3), little or no friction occurs between the contact elements (5) and the guides (2), resulting in little or no motion.
  • the micro-movement is repeated, which results in repetitive movement of the piezoresonator (3) in respect to the guides (2).
  • the exemplary piezoelectric actuators (100, 125, 150, 175) can be configured such that the guides (2) or the piezoresonators (3) provide the linear motion for the actuator. That is, either the position of the guides (2) or the piezoresonators (3) can be fixed. In the case where the position of the guides (2) is fixed, the piezoresonator (3) is attached to the stage (18) to be moved. As a result, the nano-elliptical motion of the contact elements (5) results in motion of the piezoresonator (3) and the attached stage. In contrast, in the case where the position of the piezoresonator (3) is fixed, the guides (2) are attached to the stage (18) to be moved. As a result, the nano-elliptical motion of the contact elements (5) results in motion of the guides (2) and the attached stage. In contrast to conventional piezoelectric actuators, such a configuration provides additional design flexibility.
  • the nano-elliptical motion of the contact elements (5) is formed by a superposition of two standing waves associated with orthogonal vibrational modes of the piezo-electric resonator or piezoresonator (3) such that the points of maximum vibrational velocity (9) correspond with the position of the contact elements (5). That is, the points in the piezoresonator (3) in which the standing waves of both of the orthogonal vibrational modes peak.
  • the vibrational modes are excited by providing an excitation voltage via one of a pair of electrodes (4a) and (4b) (collectively "(4)") associated with each of contact elements (5).
  • excitation voltages are provided at electrodes (4a).
  • excitation voltages are provided at electrodes (4b).
  • the excitation voltage is provided via a ground or common contact (8) and one of excitation contacts (6, 7) contacting electrodes (4b, 4a) respectively, as described below.
  • One of the vibrational modes is a longitudinal vibration resulting from a standing wave formed along a first longitudinal axis (10) along the length (L) of the piezoresonator (3).
  • the other vibrational mode is a longitudinal vibration along a second longitudinal axis (11), perpendicular to the first longitudinal axis (10) and along the width (B) of the piezoresonator (3).
  • the piezoresonator (3) combines two linear resonators- one acting along the length (L) of the piezoresonator (3) and one acting across its width (B).
  • the piezoresonator (3) is therefore effectively a 'combined resonator' in that it entails the independent and simultaneous excitation of two orthogonal oscillations to provide the nano-elliptical motion in the plane defined by the longitudinal axes (10, 11).
  • coupling between the two types of orthogonal vibrations needs to be excluded in order to provide maximum vibrational velocity for the contact elements (5).
  • energy is transferred from one vibrational mode to the other instead of energy being used for providing motion of the contact elements (5).
  • v 1 and v 2 can be mutually related in various ways depending on the geometrical parameters of the piezoresonator (3).
  • nano-ellipses (12, 13) on opposite faces of the piezoresonator (3) are also generally configured to rotate in opposite directions. This allows the piezoresonator (3) to push off the guides (2) in same direction as the contact elements (5) on both sides of the piezoresonator (3) move synchronously in the opposite directions. For example, as shown in FIGs. 1-3 , motion along nano-ellipse(s) (12) is counter-clockwise while motion along nano-ellipse(s) (13) is clockwise.
  • nano-ellipses can be excited using an excitation source operating a third frequency v 3 adjacent to v 1 and v 2 , but not coincident with either v 1 or v 2 .
  • a frequency allows formation of nano-ellipses at the central opposing maxima of vibrational velocities of the piezoresonator, assuring opposing rotation on opposite sides of the piezoresonator. Therefore, in the various embodiments of the invention, one source of alternating voltage at frequency v 3 is used to excite the two modes simultaneously without the need for a special configuration of the excitation electrodes, described above.
  • a single excitation source combination resonator is provided in the various embodiments of the invention. That is, a longitudinal resonator is provided along the length and a longitudinal resonator is provided across the width, where the same electrodes independently and simultaneously excite the two types of orthogonal vibrations.
  • FIG. 5A is an X-Y plot of frequency versus amplitude, showing the frequency response of a piezoresonator along its width and length, where the length is approximately 5 times the width.
  • the X-axis represents the excitation frequency v ex of the resonator
  • the Y-axis represents the amplitude of acoustic vibrations resulting from excitation.
  • resonant frequency v 1 corresponds to the natural resonant frequency of the longitudinal vibrations across the width of the combination resonator
  • frequency v 2 corresponds to the natural resonant frequency of longitudinal vibrations along the length of the piezoresonator.
  • an excitation frequency v 3 can selected at a point at which curves 502 and 504 substantially overlap each other.
  • v 3 is also selected by considering the phase characteristics of the resulting waves, the amplitude of excitation along the length and width can also be improved. This is illustrated with respect to FIG. 5B .
  • FIG. 5B is an X-Y plot of frequency versus phase for the system with the frequency response shown in FIG. 5A , showing the phase responses 506 and 508 of a piezoresonator along its height and width, respectively.
  • exciting the piezoresonator at or near this frequency results in an excitation of two orthogonal vibrations along the width and the length of the resonator with a difference of approximately ⁇ /2 between them.
  • the superposition of these two vibrations yields a nano-ellipse with central opposing maxima of the vibrational velocities at the sites of the contact elements. Accordingly, such a selection of v 3 allows a new methodology for simultaneous excitation of vibrational modes along both the length and width of the piezoresonator.
  • the opposite motion in the nano-ellipses (12, 13) can be provided using a single excitation voltage source by selection of the geometric dimensions of the piezoresonator (3) to provide some separation between the natural frequencies v 1 and v 2 for the piezoresonator (3) in directions parallel to the first (10) and second (11) longitudinal axes.
  • the geometric dimensions of the piezoresonator (3) are selected so that L ⁇ 2B.
  • the combined resonator frequencies are no longer the same along its orthogonal directions, but give rise to two frequencies v 1 and v 2 , where v 1 ⁇ v 2 and where v 1 and v 2 are separated according to the expression: v 1 - v 2 v 1 + v 2 / 2 * 100 % ⁇ 20 % .
  • v 1 and v 2 can be separated by 5%, 10%, 15%, or 20%.
  • a third frequency v 3 between v 1 and v 2 can be selected to excite the piezoresonator (3) that also causes nano-ellipses to be formed at the center of the opposite sides of the piezoresonator (3).
  • v 1 and v 2 can be selected such that the resulting response profiles substantially overlap, as described above with respect to FIG. 5A .
  • v 1 and v 2 can be selected such that the phase difference is ⁇ /2, as described above with respect to FIG. 5B .
  • both nano-ellipses (12, 13) are formed and they coincide with the points of maximum vibrational velocity (9) and have opposite rotations without requiring an arrangement of multiple voltage sources.
  • This approach simplifies the design of the excitation system.
  • only one source of alternating voltage with a frequency v 3 is generally necessary.
  • the excitation voltage can be applied to one of excitation contacts (6, 7) such either forward or reverse motion parallel to longitudinal axis (10) is provided.
  • this can be achieved by the excitation an appropriate one of electrodes (4a, 4b). That is, to provide motion in a first direction parallel to longitudinal axis (10), the piezoresonator is configured to generate the nano-elliptical paths for the contact elements (5) shown in FIGs. 1-3 (i.e., the counter-clockwise motion of the elliptical path (12) and the clockwise motion of the elliptical path (13)).
  • the excitation voltage is applied via excitation contact (6) to electrode (4a) and common electrode (8), while electrode (4b) is allowed to float.
  • the piezoresonator is configured to generate nano-elliptical paths for the contact elements (5) opposite to shown in FIGs. 1-3 (i.e., the clockwise motion of the elliptical path (12) and the counter-clockwise motion of the elliptical paths (13)).
  • the excitation voltage is applied only to electrode (4b) and common electrode (8) and electrode (4a) is allowed to float.
  • the piezoresonator (3) is substantially cuboid.
  • the term "cuboid”, as used herein refers to a solid figure bounded by six faces.
  • the piezoresonator can be made in the form of a rectangular plate with length L along the first longitudinal axis (10) and a width B along the second longitudinal axis (11). These surfaces bounded by width B and length L (and parallel to the longitudinal axes (10, 11)) define front (14) and back plate (15) surfaces.
  • the surfaces along length L perpendicular to the second longitudinal axis (11) define upper (16) and lower (17) surfaces of the plate.
  • the piezoresonator (3) can be polarized normal to the front and back plate surfaces (14, 15) so that the movable part of the motor allows linear movement along dimension L.
  • the contact elements (5) are positioned on the upper and lower surfaces (16, 17) of the piezoresonator.
  • the piezoresonator (3) is installed in spring-loaded guides (1, 2) which provide pressure contact between the contact sites (5) of the piezoresonator (3) and the guides (2).
  • the electrodes (4) are located in pairs (4a, 4b) on the front surface (14) the piezoresonator (3), as previously described, to provide a forward or reverse motion.
  • the first of these paired electrodes (4a) is located at positions between 2i(L/n) and (2i + 1)(L/n).
  • the second of these pair electrodes (4a) is located at positions between (2i + 1)(xL/n) and (2i + 2)(L/n). Accordingly, across the length of the piezoresonator (3), the electrodes (4a, 4b) alternate.
  • the piezoresonator (3) satisfies the conditions for formation of a second order vibrational mode along the length L, as shown in FIG. 1 .
  • a pair of contact elements (5) are located on the upper and lower surfaces (16, 17) of the piezoresonator (3), with one common electrode (8) contacting the back plate surface (15) and two others (4a, 4b) contacting the front plate surface (14). These other electrodes (4a, 4b) dividing the front surface (14) into two equal electrode areas each with length L/2, where the first electrode (4a) is connected to a first excitation contact (7), and the second electrode (4b) is connected to a second excitation contact (6).
  • the piezoresonator (3) satisfies the conditions for formation of a fourth order vibrational mode along the length L, as shown in FIG. 2 .
  • multiple pairs of contact elements (5) are located on the upper and lower surfaces (16, 17) of the piezoresonator (3), with one common electrode (8) contacting the back plate surface (15) and two pairs of electrodes (4) contacting the front plate surface (14).
  • the pairs of electrodes (4) divide the front surface (14) into four equal electrode areas each with length L/4, where the first and third electrodes (4a) are connected to each other and a first excitation contact (7), and the second and fourth electrodes (4b) are connected to each other and a second excitation contact (6).
  • the piezoresonator (3) satisfies the conditions for formation of a sixth order vibrational mode along the length L, as shown in FIG. 2 .
  • multiple pairs of contact elements (5) are located on the upper and lower surfaces (16, 17) of the piezoresonator (3), with one common electrode (8) contacting the back plate surface (15) and 3 pairs of electrodes (4) contacting the front plate surface (14).
  • These pairs of electrodes (4) divide the front surface (14) into 6 equal electrode areas each with length L/6, where the first, third, and fifth electrodes (4a) are connected to each other and a first excitation contact (7), and the second, fourth, and sixth electrodes (4b) are connected to each other and a second excitation contact (6).
  • FIGs. 6 and 7 are schematic illustrations of portions of cylindrical piezoelectric motors in accordance with other embodiments of the invention.
  • one or more piezoelectric actuators are arranged along a first longitudinal axis defined by a circular axis to provide substantially cylindrical piezoresonators in which standing acoustic waves are generated in a direction along the circular axis (first longitudinal axis) and along a second axis or direction (second longitudinal axis) substantially perpendicular to the circular axis.
  • circular axis refers to an axis defined by a circumference of a circle.
  • These piezoelectric actuators are configured similar to those shown in FIGs. 1-4 , as described below. Accordingly, the description above for components 4a, 4b, 5, 6, 7, and 8 is sufficient for purposes of describing these components in FIGs. 6 and 7 .
  • a piezoresonator 601 is provided by also disposing three piezoelectric actuators 602, 604, and 606 along a circular axis 612 about axis X. Further, the actuators 602-606 are arranged so that the contact elements 5 extend parallel to axis X. As a result, electrodes 4a and 4b are disposed on the outer surface 601a of piezoresonator 601 in a configuration similar to that of the electrodes disposed on the front surfaces in FIGs. 1-4 . Common electrode 8 is disposed on the inner surface 601b of piezoresonator 600 in a configuration similar to that of the electrodes disposed on the back surfaces in FIGs. 1-4 .
  • the length (L) of the piezoresonator 601 can be defined by the circumference of the circular axis 612 and is equivalent to the length of a linear resonator described above with respect to FIGs. 1-4 .
  • the height 614 of the piezoresonator 601 would be equivalent to the width (B) of the linear resonator, as described above with respect to FIGs. 1-4 .
  • the dimensions and excitation frequency can be selected for piezoresonator 601 in accordance with the methods described above to provide simultaneous excitation of standing longitudinal waves along directions parallel to 612 and 614 using a single excitation source applied to electrodes 4a or 4b.
  • Such a design can be used to rotate one or more rotors 616, 618.
  • a spring or other elastic component 620 can be used to bias the rotors 616 and 618 against piezoresonator 3, similar to the way the springs bias the guides against the piezoresonator in FIGs. 1-3 .
  • a parasitic radial mode of vibration can also excited.
  • a parasitic radial mode in a piezoresonator is capable of suppressing all other desired modes of vibrations in a cylindrical piezoresonator due to energy coupling. Therefore, in the embodiments of the invention using cylindrical piezoresonators, a complete or partial cut or slit 610 can be introduced halfway between two adjacent contact points 5. The slit 610 prevents the propagation of a radial mode of vibration.
  • the piezoresonator 601 can be substantially cylindrical in that in some embodiments, a complete cylinder may not be formed by the piezoresonator.
  • a piezoresonator 701 is provided by disposing three piezoelectric actuators 702, 704, and 706 along a circular axis 712 disposed about an axis X.
  • the actuators 702-706 are arranged so that the contact elements 5 extend radially with respect to axis X and perpendicular to circular axis 712.
  • electrodes 4a and 4b are disposed on the upper surface 701 a of piezoresonator 701 in a configuration similar to that of the electrodes disposed on the front surfaces in FIGs. 1-4 .
  • Common electrode 8 is disposed on the lower surface 701b of piezoresonator 700 in a configuration similar to that of the electrodes disposed on the back surfaces in FIGs. 1-4 .
  • piezoresonator 701 has a cylindrical shape, it is configured to operation as an annular or ring-type shaped piezoresonator.
  • the length (L) of the piezoresonator 701 can be defined by the circumference of the circular axis 712 and is equivalent to the length of a linear resonator described above with respect to FIGs. 1-4 .
  • the annular width 714 of the piezoresonator 701 would be equivalent to the width (B) of the linear resonator, as described above with respect to FIGs. 1-4 .
  • annular width refers to the width of an annulus or ring along a radial direction. Accordingly, the dimensions and excitation frequency can be selected for piezoresonator 701 in accordance with the methods described above to provide simultaneous excitation of standing longitudinal waves along directions parallel to 712 and 714 using a single excitation source applied to electrodes 4a or 4b.
  • a parasitic radial mode of vibration can also excited.
  • the parasitic radial mode is capable of suppressing all other desired modes of vibrations in a annular piezoresonator due to energy coupling. Therefore, in the embodiments of the invention using annular piezoresonators, a complete or partial cut or slit 710 is introduced halfway between two adjacent contact points 5. The slit 710 prevents the propagation of a radial mode of vibration.
  • the piezoresonator 701 can be substantially cylindrical in that in some embodiments, a complete cylinder may not be formed by the piezoresonator.
  • An example of an application of the motor described herein would include its incorporation as the motor element part of a micro fuel cell pump.
  • a compact, economical and quiet air pump is generally needed as part of a new generation of efficient fuel cells.
  • a rotary impeller pump using a flat piezoresonator as an actuator working on the principle of excitation of longitudinal vibrational modes along the length and the width of the piezoresonator to cause rotation of a rotor to which a fan is attached.
  • the rotary pumps described herein can be used with any type of actuator devices, including piezoresonators.
  • FIG. 8A shows a rotary pump 800 using a single fan and a piezoresonator configured in accordance with an embodiment of the present invention.
  • FIGs. 8B and 8C show top and side views, respectively, of a rotary pump 850 with two fans having opposite directions of rotation, which provides opposite direction of the airflow, a piezoresonator configured in accordance with an embodiment of the present invention.
  • the design of both pumps 800 and 850 includes: a base 51, a piezoresonator 52, rotor(s) with bearings 53, a fan 54, a spring 55, and a fuel cell element 56.
  • the rotary pumps 800 and 850 works as follows.
  • the piezoresonator 62 When the piezoresonator 62 is electrically excited, its ends vibrate following an elliptical locus of movement, with the plane of this movement being parallel to the major plane of the piezoresonator 62.
  • the elliptical path of the vibrations results from the combination of the deformations of the piezoresonator 62, stimulated by the electrical excitation of the piezoresonator 62.
  • the end(s) of the piezoresonator 62 are held under the pressure of the spring 55 against the rotor(s) 53, so that the elliptical movement of the ends of the piezoresonator 52 transmits, via friction at the piezoresonator/rotor(s) contact area(s), rotation of the rotor(s) 53, which in turn causes the fan(s) 54 to rotate.
  • the air from the fan(s) 54 is directed to the fuel cell element 56 to provide the oxygen for its operation.
  • the thickness of the piezoresonator 52 is less than 2 mm, and the rotary pump 600 would occupy a space in the order of 2 - 4 cm 3 enabling it to be fitted fit into a square area of side 25 mm.
  • the two-fan design shown in FIGs. 8B and 8C , provides an increased airflow and greater efficiency in the supply of air to the fuel cell. This design is intrinsically energy efficient and depending on the quality of the rotor bearing could be practically noiseless.

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  • General Electrical Machinery Utilizing Piezoelectricity, Electrostriction Or Magnetostriction (AREA)
  • Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)

Claims (13)

  1. Piezoelektrische Vorrichtung, die aufweist:
    einen Piezoschwingkörper (3) mit einer ersten Fläche (14) und einer zweiten Fläche (15), die einander entgegengesetzt angeordnet sind, und einer dritten Fläche (16) und einer vierten Fläche (17), die einander entgegengesetzt angeordnet sind, wobei die erste Fläche und die zweite Fläche im Wesentlichen parallel zu einer ersten Längsachse (10) und einer zweiten Längsachse (11) des Piezoschwingkörpers angeordnet sind, und die dritte Fläche und die vierte Fläche im Wesentlichen parallel zu der ersten Längsachse und im Wesentlichen rechtwinklig zu der zweiten Längsachse angeordnet sind, und wobei die erste Längsachse und die zweite Längsachse im Wesentlichen rechtwinklig zueinander angeordnet sind;
    mindestens eine gemeinsame Elektrode (8), die auf der zweiten Fläche angeordnet ist;
    eine Mehrzahl von Elektroden (4a, 4b), die auf der ersten Fläche angeordnet sind, wobei die Mehrzahl von Elektroden ein Paar oder mehrere Paare von Anregungselektroden aufweisen, wobei jedes der Paare von Anregungselektroden eine erste Elektrode und eine zweite Elektrode aufweist, die entlang einer ersten Richtung entlang der ersten Längsachse angeordnet sind;
    ein Kontaktelement (5) oder mehrere Kontaktelemente (5), das/die an mindestens einer der dritten Fläche und der vierten Fläche an einem Kontaktort oder mehreren Kontaktorten angeordnet ist/sind, wobei jeder der Kontaktorte zumindest teilweise zwischen der ersten Elektrode und der zweiten Elektrode eines der genannten Paare von Anregungselektroden angeordnet ist; und
    eine Wechselspannungsquelle, wobei die Wechselspannungsquelle dazu eingerichtet ist, eine Wechselspannung an die gemeinsame Elektrode und an eine der ersten Elektrode und der zweiten Elektrode in jedem der genannten Paare von Anregungselektroden anzulegen, um eine nano-elliptische Bewegung zumindest eines Teils der Kontaktelemente zu bewirken, wobei die nano-elliptische Bewegung im Wesentlichen parallel zu der ersten Fläche und der zweiten Fläche erfolgt, wobei die nano-elliptische Bewegung des Teils der an der dritten Fläche angeordneten Kontaktelemente in einem ersten elliptischen Pfad erfolgt, wobei die nano-elliptische Bewegung des Teils der an der vierten Fläche angeordneten Kontaktelemente in einem zweiten elliptischen Pfad erfolgt, der dem ersten elliptischen Pfad entgegengesetzt ist;
    wobei der piezoelektrische Körper eine natürliche Resonanzfrequenz (v 1) für eine erste stehende Längswelle in eine Richtung der zweiten Längsachse aufweist, eine natürliche Resonanzfrequenz (v 2) gerader Ordnung für eine zweite stehende Längswelle in eine Richtung der ersten Längsachse aufweist, wobei: 0 % < v 1 - v 2 v 1 + v 2 / 2 * 100 % ≤ 20 % ;
    Figure imgb0008
     und
    wobei eine Frequenz ( v 3 ) der Wechselspannungsquelle zwischen v 1 und v 2 beträgt.
  2. Piezoelektrische Vorrichtung nach Anspruch 1, bei der der piezoelektrische Körper eine Länge (L) entlang der ersten Längsachse aufweist, eine Breite (B) entlang der zweiten Längsachse aufweist, und bei dem B = C/(2v 1) und L = (nC)/(2v 2) gilt, wobei C die Schallwellengeschwindigkeit in dem Piezoschwingkörper ist, n = 2k beträgt, und k eine ganze Zahl ≥1 ist.
  3. Piezoelektrische Vorrichtung nach Anspruch 2, bei der eine erste Anregungselektrode jedes Paares der Anregungselektroden in je einem ersten Elektrodenbereich entlang L zwischen 2i(L/n) und (2i + 1)(L/n) angeordnet ist, und bei dem eine zweite Anregungselektrode jedes Paares von Anregungselektroden in je einem zweiten Elektrodenbereich entlang L zwischen (2i +1)(L/n) und (2i + 2)(L/n) angeordnet ist, wobei i eine ganze Zahl ist und (n-2)/2 ≥ i ≥ 0 gilt.
  4. Piezoelektrische Vorrichtung nach Anspruch 3, bei der die Kontaktorte für die Mehrzahl von Kontaktelemente durch (2i +1)(L/n) definiert sind.
  5. Piezoelektrische Vorrichtung nach Anspruch 4, bei der n = 2 ist.
  6. Piezoelektrische Vorrichtung nach Anspruch 4, bei der n = 4 ist.
  7. Piezoelektrische Vorrichtung nach Anspruch 4, bei der n = 6 ist.
  8. Piezoelektrische Vorrichtung nach Anspruch 1, die ferner mindestens eine obere Führung aufweist, die über der oberen Fläche angeordnet ist, und die mindestens eine untere Führung aufweist, die unter der unteren Fläche angeordnet ist, wobei die obere Führung und die untere Führung derart angeordnet sind, dass sie sich während eines Abschnitts der nanoelliptischen Bewegung in physischem Kontakt mit den Kontaktelementen befinden, wobei die obere Führung und die untere Führung während des physischen Kontakts elastisch gegen die Kontaktelemente vorgespannt sind.
  9. Piezoelektrische Vorrichtung nach Anspruch 8, die ferner eine Plattform aufweist, und bei der der Piezoschwingkörper oder die obere Führung oder die untere Führung bezüglich der Plattform eine feste Stellung aufweist/aufweisen.
  10. Piezoelektrische Vorrichtung nach Anspruch 1, bei der der Piezoschwingkörper im Wesentlichen kubusförmig ist.
  11. Piezoelektrische Vorrichtung nach Anspruch 1, bei der der Piezoschwingkörper eine im Wesentlichen zylindrische Form aufweist.
  12. Piezoelektrische Vorrichtung nach Anspruch 11, bei der der Piezoschwingkörper einen Schlitz aufweist, wobei sich der Schlitz zumindest zum Teil in eine Richtung quer zu der ersten Längsachse erstreckt.
  13. Piezoelektrische Vorrichtung nach Anspruch 1, bei der der Piezoschwingkörper und die Mehrzahl von Kontaktelementen integral ausgebildet sind.
EP09838002.5A 2008-12-18 2009-12-18 Piezoelektrische quasi-resonanzmotoren auf der basis von akustischen stehwellen mit kombiniertem resonator Active EP2374205B1 (de)

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US8299684B2 (en) 2012-10-30
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US8710719B2 (en) 2014-04-29
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US20100156239A1 (en) 2010-06-24
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